Related Experiment Video
Updated: Feb 15, 2026

10:00
Gradient Echo Quantum Memory in Warm Atomic Vapor
Published on: November 11, 2013
13.3K
Quantum Triple Point and Quantum Critical End Points in Metallic Magnets
1Department of Physics and Theoretical Science Institute, University of Oregon, Eugene, Oregon 97403, USA.
Physical Review Letters
|January 13, 2018
Summary
Quantum effects significantly alter magnetic phase diagrams. They reduce areas of concurrent ferromagnetic (FM) and antiferromagnetic (AFM) order and change magnetic transitions, revealing new quantum critical points.
Area of Science:
- Condensed matter physics
- Quantum magnetism
Background:
- Ferromagnetic (FM) and antiferromagnetic (AFM) orders are fundamental in low-temperature metallic magnets.
- Classical magnet phase diagrams describe the coexistence and transitions between these magnetic orders.
Purpose of the Study:
- To investigate the impact of universal quantum effects on the phase diagrams of metallic magnets.
- To understand how quantum phenomena modify the regions of concurrent FM and AFM order and the nature of magnetic transitions.
Main Methods:
- Theoretical analysis of magnetic systems incorporating quantum effects.
- Phase diagram mapping under varying conditions, including the presence of a magnetic field.
Main Results:
- Quantum effects qualitatively alter classical magnet phase diagrams.
- The region of concurrent FM and AFM order is reduced.
- Several magnetic transitions change from second-order to first-order.
- A quantum triple point or a quantum critical end point emerges in a magnetic field.
Conclusions:
- Universal quantum effects play a crucial role in shaping the low-temperature phase diagrams of metallic magnets.
- These quantum effects lead to novel phase behaviors, including new types of critical points.
Related Concept Videos
Quantum Numbers
52.4K
It is said that the energy of an electron in an atom is quantized; that is, it can be equal only to certain specific values and can jump from one energy level to another but not transition smoothly or stay between these levels.
52.4K
The Quantum-Mechanical Model of an Atom
59.8K
Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
59.8K
2D NMR: Heteronuclear Single-Quantum Correlation Spectroscopy (HSQC)
1.5K
Heteronuclear single-quantum correlation spectroscopy (HSQC) is a 2D NMR technique that reveals one-bond correlations between hydrogen and a heteronucleus. The HSQC experiment is similar to the heteronuclear correlation experiment (HETCOR) but is more sensitive. In the HSQC spectrum, the proton chemical shift is plotted on the horizontal F2 axis, while the 13C chemical shift is plotted on the vertical F1 axis. The corresponding proton and 13C spectra are also shown. The HSQC contour plot does...
1.5K
Properties of Transition Metals
30.1K
Transition metals are defined as those elements that have partially filled d orbitals. As shown in Figure 1, the d-block elements in groups 3–12 are transition elements. The f-block elements, also called inner transition metals (the lanthanides and actinides), also meet this criterion because the d orbital is partially occupied before the f orbitals.
30.1K
Bonding in Metals
53.0K
Metallic bonds are formed between two metal atoms. A simplified model to describe metallic bonding has been developed by Paul Drüde called the “Electron Sea Model”.
53.0K
Metallic Solids
21.0K
Metallic solids such as crystals of copper, aluminum, and iron are formed by metal atoms. The structure of metallic crystals is often described as a uniform distribution of atomic nuclei within a “sea” of delocalized electrons. The atoms within such a metallic solid are held together by a unique force known as metallic bonding that gives rise to many useful and varied bulk properties.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability....
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability....
21.0K

